The interpolating operator of top partner chimera baryon has been written down in Ref. [1]}. One uses \((\Gamma ^1,\,\Gamma ^2)\equiv (C\gamma ^5,\,\mathbb {1})\) . Other choices of gamma matrices can be found in Ref. [2]} for the \(SU(4)\)  gauge theory. In analogy with QCD, we denote as \(\Lambda \)  the state with quantum numbers \((J,R) = (1/2,5)\) , where \(J\)  is the spin and \(R\)  denotes the irreducible representation of the flavour group acting on \(Q^i\) . This state provides a natural candidate as a top partner [3]}. At large Euclidean time, the 2-point correlation function for this \(\Lambda \) -type operator asymptotically behaves as
\(C(t) \xrightarrow{} P_e \left[ c_ee^{-m_et} + c_oe^{-m_o(T-t)} \right] - P_o \left[ c_oe^{-m_ot} + c_ee^{-m_e(T-t)} \right],\) 
